US2999978A

US2999978A - Nuclear magnetic resonance measuring apparatus

Info

Publication number: US2999978A
Application number: US862361A
Authority: US
Inventors: Clyde W Pinkley
Original assignee: Industrial Nucleonics Corp
Current assignee: Industrial Nucleonics Corp
Priority date: 1959-12-28
Filing date: 1959-12-28
Publication date: 1961-09-12
Anticipated expiration: 1978-09-12

Description

Sept. 12, 1961 c. w. PINKLEY NUCLEAR MAGNETIC RESONANCE MEASURING APPARATUS Filed Dec. 28. 1959 2 Sheets-Sheet 1 m P C FPl.| U M F a .S E R T F E A D w E P e m I. M w L C S O u m {L INVENTOR Sept. 12, 1961 c. w. PINKLEY 2,999,978

NUCLEAR MAGNETIC RESONANCE MEASURING APPARATUS Filed Dec. 28. 1959 2 Sheets-Sheet 2 2 HA H8 p- LIJ con. A 0.5R con. B

DISTANCE BETWEEN COILS 7y 6 K Q IINVENTOR M 5 4 Aim United States Patent 2,999,978 NUCLEAR MAGNETIC RESONANCE MEASURING APPARATUS Clyde W. Pinkley, Columbus, Ohio, assignor to Industrial Nucleonics Corporation, a corporation of Ohio Filed Dec. 28, 1959, Ser. No. 862,361 '10 Claims. (Cl. 324-.5)

This invention relates to measuring apparatus, and in particular to an improved magnet and coil assembly for conditioning flat sheet material to be analyzed by measurement of various phenomena occurring in response to nuclear magnetic resonance.

It is well known in the prior art relating to nuclear physics that many atomic nuclei possess magnetic moment and nuclear momentum or spin. A nucleus having these characteristics displays gyroscopic eifects and is therefore often considered analogous to a spinning gyroscope having a magnet positioned along its axis.

When such nuclei are subjected to a constant uniform external magnetic field, the spinning nuclei tend to precess around an axis parallel to the magnetic field with a characteristic frequency and with random phase. Initially the resulting polarization is zero, but, after a characteristic time, damping forces cause an excess of nuclei to exhibit a magnetic component in the direction of the external field. In the event the polarized nuclei are subjected to a radio-frequency magnetic field at right angles to the external field and at the frequency of nuclear precession, phase coherence is introduced among the nuclei with the result that the induced polarization precesses about the external field direction with a corresponding loss of energy in the radio-frequency field.

Prior investigators have studied the gyroscopic properties of nuclei by subjecting an element to a magnetic field produced by a permanent magnet or electromagnet and simultaneously irradiating the element with radio-frequency electromagnetic energy emanating from a tank coil.

When the frequency of the radio-frequency source resonates with the frequency of nuclear precession, the spinning nuclei absorb a maximum amount of energy from the radio-frequency field thereby loading the tank circuit. It has been determined that the resonant frequency of nuclear precession varies for different elements and for different values of the polarizing magnetic field.

Within recent years, measuring devices have been proposed operative in response to the energy absorption occurring at the nuclear magnetic resonance frequency. From this absorption measurement, the relative proportion of an element in question can be determined because the total energy absorbed is a function of the number of nuclei present, other things being equal. Apparatus of this type can be used for the quantitative determination of any element the nucleus of which possesses angular momentum and magnetic moment, such as for example, H H He Li Li Be B B N etc. Additionally, quantitative determination of numerous isotopes of elements can also be made, because in all cases the diiferent isotopes possessing non-zero magnetic moments have dilferent resonant frequencies in the same external field.

The absorption phenomenon of nuclear magnetic resonance is also used to measure constituent proportions in various compounds. For example, moisture content measurements can be made in materials, such as tobacco or paper. In such a determination the water content is not measured directly but, rather, the hydrogen in the material is distinguished from the hydrogen in water on the basis of widely difiering absorption patterns. By applying the same principles it is possible to measure the presence of any compound which contains at least one ele- Patented Sept. 12, l96l ment the nucleus of which possesses angular momentum and magnetic moment.

In one type of conventional nuclear magnetic resonance apparatus, radio-frequency current from a constant-current source is supplied to a parallel tuned circuit consisting of a coil and capacitor. The tank coil, ordinarily a solenoid is placed within the uniform external field of a permanent magnet so that the radio-frequency field is perpendicular to the external field, and the material to be measured is placed within the coil.

The frequency of the radio-frequency field, or the magnitude of the external field, is modulated at a slow audio rate. When the radio-frequency and the magnetic fields satisfy the relation W ='yH whereW is the angular velocity of the radio-frequency field H H is the permanent magnetic field strength in gauss, and y is a constant dependent on the type of nucleus subjected to resonance, nuclear magnetic resonance occurs.

The resulting nuclear resonance causes a decrease in the impedance of the tank circuit, and therefore a decrease in the voltage appearing across the tank circuit. For a given set of conditions the magnitude of this change in voltage is proportional to the amount of absorbing substance present so that a quantitative measurement can be made.

With a given amount of absorbing substance, the magnitude of voltage change is proportional to the radiofrequency field strength provided that saturation does not occur. It is therefore desirable to maintain the field strength to as high a value as possible without attaining saturation.

The use of nuclear magnetic resonance for the measurement of moisture or other characteristics of sheet material presents the problem of subjecting a cross section of the sheet to the mutually perpendicular radio-frequency and external fields which satisfy the requirements for nuclear resonance. Since it is physically impossible to place a large sheet of material within a radio-frequency coil of the solenoidal type where the field has its highest, most uniform concentration, the sheet in many prior art arrangements is subjected to the field extending from the end of the coil (where the field is dispersed) thus greatly decreasing the sensitivity of the measuring device.

The disposition of the pole pieces required to generate a magnetic field H perpendicular to the radio-frequency field H has also dictated several compromise magnet and coil assemblies Which have resulted in relatively poor signal-to-noise ratios in the measurement of sheet material.

Additionally, optimum signal-to-noise ratios and accurate measurements are obtained when the largest possible portion of the total radio-frequency field H is placed in the sheet portion under test, or in other words a high filling factor is desired. Another important requirement is to obtain a radio-frequency field H that is reasonably uniform with respect to possible changes in the relative position of the test sample. In the case of a continuous flat sheet, this undesirable change in relative position is,

attained by movement in a direction perpendicular to the sheet. Magnet and coil assemblies heretofore employed have not provided fully satisfactory measurements in sheet material because of the inability to adequately meet these requirements.

Accordingly, a principal object of this invention is to:

improve the signal-to-noise ratio and the sensitivity of nuclear magnetic resonance sheet measuring apparatus.

Another object is to provide an improved magnet and coil assembly for nuclear magnetic resonance measuring apparatus that is advantageously adapted for the testing of sheet material.

Another object is to provide a magnet and coil assembly of substantially improved efiiciency for nuclear magnetic resonance measuring apparatus thatsubjects the material under test to higher external field intensities of better homogeneity.

A preferred embodiment of the magnet and coil assembly of this invention comprises a modified Helmholtz pair of coils disposed between a pair of spaced magnet pole pieces. The coils are axially aligned and closely spaced in a parallel relationship with respect to one another. Both coils are included in a resonant tank circuit that develops an output signal in response to a condition of nuclear magnetic resonance in sheet material positioned between the coils.

The coils are connected in -a reverse sense so that their respective radio-frequency magnetic fields are in opposition or bucking. This connection provides radio-frequency magnetic flux between the two coils which is essentially radial to the common axis of the two coils except at points near the axis and beyond the outer perimeter of the coils. The sample sheet under test is preferably disposed in the median plane between the coils that is perpendicular to the common axis of the coils. The resulting lines of flux emanating from the two coils thus lie in the plane of the material under test.

Due to the increased flux density between the coils a satisfactory filling factor is obtained with coil spacings of a few sample thicknesses.

A principal novel feature of this invention is directed to the construction details for both coil windings. The distance between corresponding turns on the two coils is equal to the radius of the turns. With this geometry, the rate of change of magnetic field with distance from the plane of a given coil is a constant at a point equal to one-half the radius of the coil. .Inasmuch as two coils are used, one on each side of this point, the de crease in field of one coil is balanced by the increase in field of the other so that the combined field will be very nearly constant. The primary improvement over previous fiat coil designs is the improvement in radiofrequency field uniformity between the coils and the increase in size of the uniform region for a given coil size.

In order that all of the features for attaining the objects of this invention may be readily understood, reference is herein made to the drawings wherein:

FIG. 1 is a simplified circuit diagram of nuclear magnetic resonance measuring apparatus employing the improved magnet and radio-frequency coil assembly of this invention;

'FIG. 2 is a perspective view showing the improved arrangement herein of the magnet pole pieces and the radio-frequency coils relative a sheet of material under test;

FIG. 3 is a cross-sectional view of the magnetic and radio-frequency fields generated by the radio-frequency coils of FIG. 2;

FIG. 4 is a diagram of the radial components of the radio-frequency field generated in the view of FIG. 3;

FIG. 5 is a diagram of assistance in showing the relationship between the radius of the coil turns and the distance separating corresponding coil turns; and

FIG. 6 is a set of curves showing various field strength curves for a pair of single turn coils designed in accordance with the requirements of FIG. 5.

Referring now to the simplified showing of the measuring apparatus of FIG. 1 incorporating the magnet and coil assembly of this invention, sheet material 10 under test is positioned midway between radio-frequency sampling coils 11 and 12. The coils 11 and 12 are axially aligned and disposed in a parallel relationship with respect to one another. For reasons hereinafter outlined in detail, material 10 is subjected to a radio-frequency field H radial to the axis of the coils and within the plane containing the sheet. Material 10 is also subjected to a magnetic field H developed in the gap between

external magnets

13 and 14. Field H is perpendicular to the radial components of the radio-frequency field H Modulation coils 15 and 16 envelope the pole ends of magnets .13 and 14, respectively, so that the otherwise steady magnetic field is amplitude modulated by the audio-frequency energy supplied from modulation source 17.

Capacitor 18 shunts coils 11 and 12 so that the

combination

11, 12, 18 forms a parallel-resonant tank circuit connected to the output of constant-current radiofrequency oscillator 19. Other circuit arrangements may be apparent such as connecting coils 11 and 12 in parallel with the connection to the condenser 18 either in series or in parallel. Alternately the coils 11 and 12 may @be independently resonated with two separate condensers and coupled together in an opposing sense by means of identical transmission lines from a common radio-frequency source properly matched in impedance to the source and to the resonant circuits.

The tank circuit is tuned to the oscillator frequency and therefore a substantial radio-frequency voltage appears across the tank circuit. This voltage has a constant amplitude except during those periodic instances at which the output frequency of oscillator 19 and the modulated magnetic field generated by the magnets 13 and14 and modulation coils 15 and 16 satisfy the requirements for nuclear resonance.

During resonance, material 10 absorbs energy from the radio-frequency field so 'as to periodically load coils 11 and 12. As is well known, the loading of a parallel tank circuit lowers the Q of the tank, thereby reducing the parallel impedance appearing across the tank circuit. The periodic absorption of energy by material It thus amplitude modulates the radio-frequency voltage appearing across

tank circuit

11, 12, 18. The am plitude of this modulation component varies in accordance with .the number of nuclei present in the material 10 to absorb energy from tank coils 11 and 12.

The voltage appearing across

tank circuit

11, 12, 18 is applied to the input of radio-frequency amplifier 20. The signal output of radio-frequency amplifier 20 is in turn applied to the input of detector and audio-frequency amplifier 21. This latter unit develops an audio-frequency signal corresponding to the modulation component introduced'by absorption variations in material 10. This signal is applied to the vertical amplifier of oscilloscope 22.

The horizontal sweep of oscilloscope 22 is synchronized to the periodic vertical voltage pulses by applying a voltage from modulation source 17 to appropriate horizontal sweep terminals of the oscilloscope. Accordingly, a stationary pulse appears on the screen of the oscilloscope which has an amplitude responsive to variations in the absorption characteristics of thematerial 10 under test.

An enlarged perspective view of the magnet and coil assembly of this invention is shown in FIG. 2. Sheet 10 is disposed midway between the faces of the

magnet pole pieces

13 and 14 and also midway between the adjacent end surfaces of radio-frequency coils 11 and 12. The sheet moves in a plane parallel to the adjacent faces of the magnet pole pieces and also the adjacent surfaces of radio-frequency 'coils 11 and '12. Conventional means may be employed for moving sheet 10 throughout the required plane, the essential requirement being that the sheet preferably be maintained in the relative position set forth.

Radio-frequency coils 1 1 and 1.2 are spiral-wound as hereinafter outlined in detail so that end openings 25 and 26 are formed therein, respectively. The two coils 11 and 12 may both be real physical coils as shown or one of the coils and its associated radio-frequency field-may be an electricalimage of the other real physical coil, the electrical image being formed by the well known method of placing a metallic conducting sheet in the position of the median plane. In this case the sample sheet must be slightly displaced from the median plane in the directionof the physical coil.

It should .be noted that coils 11 and Hate reversely connected inasmuch as conductor 27 connects the upper center output lead of coil 12 with the corresponding lead of coil 11. Output connections to both reversely connected coils 11 and 12 are made to the

outer conductors

28 and 29. Capacitor 18 is connected across

conductors

28 and 29 so that a parallel resonant tank combination 11, 12, "18 is formed.

The steady magnetic field H generated by

magnet pole pieces

13 and 14 is parallel to the common longitudinal axis 35 of coils 11 and 12 and perpendicular to the surfaces of sheet 10. Modulation coils 15 and 16 are wound around the terminal ends of the

pole pieces

13 and 14, respectively, so that the otherwise steady magnetic field H may be amplitude modulated.

FIG. 3 shows a diagram of the fields H and H generated by the magnet pole pieces 113 and 14 and radiofrequency coils 11 and 12. The X-marked conductors '30 of coil 11 and the X-marked conductors 31 of coil 12 are those conductors in which current flows into the plane of the figure, and the plain conductors 32 of coil 11 and the plain conductors 33 of coil 12 are those conductors in which current flows out of the plane of the figure. The conductor group 30, therefore, generates clockwise flux loops and conductor group 33 generates counterclockwise flux loops. Accordingly, the lowermost flux lines generated by conductor group 30 and the uppermost flux lines generated by conductor group 33 combine to develop reinforcing resulting flux lines which are parallel to the plane of sheet 10 and directed to the left of the figure.

Conductor group 32 generates counter-clockwise flux loops and conductor group 31 generates clockwise fiux loops. Accordingly, the lowermost fiux lines generated by group 32 and the uppermost flux lines generated by group 31 combine to form reinforcing resulting lines which are in the plane of sheet 10. These resulting lines are directed to the right of the figure.

The foregoing magnet and coil assembly thus generates radio-frequency flux between the two coils 11 and 12 which is essentially radial to the common axis 35 of the two coils as is shown in FIG. 4, except at points near the axis 35 of the two coils and beyond the outer perimeter.

As is best shown in FIG. 5, coils 11 and 12 are identical and are so wound that the distance between corresponding turns on the two coils equals the radius of the turns. For example, the individual turns on coils 11 and 12 having a radius of M1 are separated from one another by a like distance M1. Likewise, the individual turns of coils 11 and 12 that have a radius M2 are separated from one another by the distance M2.

For a single turn coil, the rate of change of magnetic field strength with distance from the plane of the coil is a constant at a point equal to one-half the radius of the coil. In the event two coils are used, one on each side of the point, the decrease in field of one coil will be balanced by the increase in field of the other so that the combined field will be very nearly constant.

The above relationship is shown in the graph of FIG. 6 wherein the relative field strengths for two identical single turn coils A and B are shown plotted with respect to the distance between the coils in fractions of one radius. The coils are located in parallel planes spaced at a distance of one radius. Curve HA shows that the magnetic field strength is a maximum in the plane of coil A, and that this field strength varies at a constant, decreasing value at a distance of approximately 0.5 radius from coil A. Likewise, curve HB shows that the magnetic field strength of coil B is at a maximum in the plane of coil B, and this field strength decreases at the same rate that the field strength of coil A increases when measured at a distance of 0.5 radius from coil B.

Accordingly, it may be readily seen that the decrease in field strength of one coil is balanced by the increase in the field strength of the other coil. The combined field strength for both coils A and B is shown in curve HA+HB. In view of the fact that this composite curve 6 is relatively fiat in the region, from say, 0.3 to 0.7 radius, variations in the position of a sheet under test between magnet pole pieces within this radius range will not be accompanied by variations in radio-frequency field strength.

Accordingly, the particular design of coils 11 and 12 shown herein gives very good radio-frequency field uniformity throughout the region between the coils and allows more movement of the sheet in this region without affecting the sensitivity. In addition to the improvement in radio-frequency field uniformity between coils 11 and 12, there is also a corresponding increase in the size of the uniform region for a given coil size.

It should be understood that the above described arrangements are merely illustrative of the features of this invention and that numerous other arrangements may be devised without departing from this scope of the invention.

What is claimed is:

1. In nuclear magnetic resonance measuring apparatus for subjecting flat sheet material to be analyzed to mutually perpendicular magnetic and radio-frequency fields including a resonant tank circuit developing an output signal responsive to a condition of nuclear resonance between the fields and for the material under measurement, the improvement comprising a pair of identical coils axially aligned and spaced with respect to one another so that the distance between corresponding turns on the two coils equals the radius of the turns, a radiofrequency source energizing said coils to produce opposing radio-frequency magnetic fields in the common space therebetween and as measured along the axis, means adapted to support the fiat sheet material under measurement in the space between the coils, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the axis thereof.

2. In nuclear magnetic resonance measuring apparatus for subjecting flat sheet material to be analyzed to mutually perpendicular magnetic and radio-frequency fields including a resonance tank circuit developing an output signal responsive to a condition to nuclear resonance between the fields and for the material under measurement, the improvement comprising a pair of substantially identical coils axially aligned and spaced with respect to one another so that each coil is an image of one another in a median plane therebetween, both of said coils being included in said resonant tank circuit and wound so that corresponding turns on both coils have an increasing radius as the distance thereof from the median plane is increased, a radio-frequency source energizing said coils to produce opposing radio-frequency magnetic fields in the common space therebetween and as measured along the axis, means adapted to support the fiat sheet material under measurement midway between the coils and perpendicular to the axis thereof, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the axis thereof.

3. In a measuring system substantially as set forth in claim 2 wherein one of said coils is a real physical coil and the other is means providing an electrical image of the physical coil.

4. In a nuclear magnetic resonance measuring apparatus for subjecting a material to be analyzed to mutually perpendicular magnetic and radio-frequency fields including a resonant tank circuit developing an output signal responsive to a condition of nuclear resonance between the fields and for the material under measurement, the improvement comprising a pair of substantially identical coils disposed on a common axis and connected relative one another to develop opposing magnetic fields in the space between the coils and generating reinforcing resulting lines of magnetic flux radially emanating from said axis, each of said coils being wound so that the distance between corresponding turns on the two coils equals the radius of the turns, -a radio-frequency Source energizing both of said coils, means adapted -.to support the material under measurement in the spacetbetween the coils, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the common axis thereof.

5. In a measuring system substantially as set forth in claim 4 wherein one of said coils is a real physical .coil and the other is means providing an electrical image of the physical coil.

6. In nuclear magnetic resonance measuring apparatus for subjecting a material to be analyzed to mutually perpendicular magnetic andradio-frequency fields including a resonant tank circuit developing an output voltage responsive to a condition of nuclear resonance between the fields and for the material under measurement, the improvement comprising a pair of identical coils each formed with a center opening and included in said resonant tank circuit, said coils being in a spaced relationship with respect to one another and symmetrically disposed on a common axis passing through the center of said coils, each of said coils'being wound so'that the distance between corresponding turns on the two coils equals the radius of the turns, a radio-frequency source energizing said coils to produce opposing radio-frequency magnetic fields in the common space therehetween having reinforcing resulting components radially emanating from said axis, means adapted to support the material under measurement in the space between the coils, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the axis thereof.

'7. In nuclear magnetic resonance measuring apparatus for subjecting fiat sheet material to' be analyzed to.mutually perpendicular magnetic and radio-frequency fields including a resonant tank circuit developing an output voltage responsive to a condition of nuclear resonance between the fields and for the material under measurement, the improvement comprising a pair of identical coils each formed with a center opening and including in said resonant tank circuit, said coils being in .a spaced relationship with respect to one another and symmetrically disposed on a common axis passing through the center of said coils, so that each coil is an image of one another in a median plane therebetween, each of .said coils being wound so that corresponding turns on both coils have an increasing radius as .the distance thereof from the median plane is increased, a radio-frequency source energizing said coils to produce opposing radiofrequency magnetic fields in the common space there between having reinforcing resulting components radially emanating from said axis, means adapted to support the sheet material under measurement midway between the coils and perpendicular to axis, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the axis thereof.

8. In nuclear magnetic resonance measuring apparatus for subjecting a material to be analyzed to mutually perpendicular magnetic and radio-frequency fields, including a resonant tank circuit developing an output signal responsive to a condition of nuclear resonance between the fields and for the material under measurement, and having a pair of identical coilsaxially aligned and spaced 8 r r so that each coil is an image of one another, a radiofrequency source energizing said coils to produce opposing radio-frequency magnetic fields in the commonspace therebetween and as measured along the axis, means adapted to support the material under measurement in the space between the coils, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the axis thereof, the improvement .comprising each of said coils being wound so that corresponding turns on both coils have an increasing radius as the distance thereof from the median plane is increased.

9. In nuclear magnetic resonance measuring apparatus for subjecting a material to be analyzed to mutually perpendicular magnetic and radio-frequency fields, including a resonant tank circuit developing an output signal responsive to a condition of nuclear resonance between the fields and for the material under measurement, a pair of coils disposed on a common axis and connected relative one another to develop opposing magnetic fields in the space between the coils and generating reinforcing resulting lines of magnetic flux radially emanating from said axis, a radio frequency source energizing both of said coils, means adapted to support the coils, and a pair of spaced magnet poles developing a second magnetic field passing through said coils and parallel to the common axis thereof, the improvement comprising each of said coils being wound so that corresponding turns on both coils have an increasing radius as the distance thereof from the median plane therebetween .is increased.

10. In nuclear magnetic resonance measuring apparatus for subjecting a material to be analyzed to mutually perpendicular magnetic and radio-frequency fields, including a resonant tank circuit developing an output signal responsive to a condition of nuclear resonance between the fields and for the material undermeasurement, a pair of coils disposed on a common axis and connected relative one another to develop opposing magnetic fields in the space between the coils and generating reinforcing resulting .lines of magnetic flux radially emanating from said axis, a radio frequency source energizing both of said coils, means adapted to support thematerial under measurement in the space between the coils, and a pair of spaced magnetpoles developing a second magnetic field passing through said coils and parallel to the common axis thereof, the improvement comprising each of said coils being wound so that the distance between corresponding turns on the two coils equals the radius of the turns.

References Cited in the file of this patent FOREIGN PATENTS Great Britain Nov. 24, 1932 France Mar. 18, 1957 OTHER REFERENCES